2.5 Limits at Infinity

Total Page:16

File Type:pdf, Size:1020Kb

2.5 Limits at Infinity For Use Only in 2013 2014– Pilot Program 96 Chapter 2 r Limits 46–47. Steep secant lines b. Create a graph that gives a more complete representation of f. a. Given the graph of f in the following figures, find the slope of the 1 2 1 1 22 y secant line that passes through 0, 0 and h, f h in terms of h, for h 7 0 and h 6 0. 20 b. Evaluate the limit of the slope of the secant line found in part (a) as h S 0+ and h S 0-. What does this tell you about the line tangent to the curve at 10, 02? 15 1 2 = 1>3 46. f x x ϭ 2000 10 y y 50 ϩ 100 x2 5 (h, h1/3) (0, 0) Ϫ4 Ϫ2 420 x h x y ϭ x1/3 Technology Exercises T 49–56. Asymptotes Use analytical methods and/or a graphing utility to identify the vertical asymptotes (if any) of the following functions. x2 - 3x + 2 2>3 1 2 = 1 2 = - 2 1 2 = 47. f x x 49. f x 50. g x 2 ln x x10 - x9 y x p 1 2 = e 1 2 = a xb ͉ ͉ 6 y ϭ x2/3 51. h x 52. p x sec , for x 2 1x + 123 2 (h, h2/3) pu p 53. g1u2 = tan a b 54. q1s2 = (0, 0) 10 s - sin s h x 1 2 = 1 1 2 = 1>x 55. f x 56. g x e 1x sec x T 57. Can a graph intersect a vertical asymptote? A common mis- conception is that the graph of a function never intersects its verti- cal asymptotes. Let T 48. Care with graphing The figure shows the graph of the function 1 2 = 2000 3 - 4 * 3 4 4 6 f x graphed in the window 4, 4 0, 20 . if x 1 2 1 2 = - 50 + 100x f x W x 1 2 Ú . 1 2 1 2 1 2 x if x 1 a. Evaluate lim f x , lim f x , and lim f x . xS0+ xS0- xS0 Explain why x = 1 is a vertical asymptote of the graph of f and show that the graph of f intersects the line x = 1. QUICK CHECK ANSWERS 1. Answers will vary, but all graphs should have a vertical asymptote at x = 2. 2. - ∞; ∞ 3. As x S -4+ , x 6 0 and 1 + 2 7 1 + 2 S x 4 0, so x x 4 0 through negative values. 1x - 121x - 22 = 1 - 2 = 4. lim lim x 1 1, which is not xS2 x - 2 xS2 an infinite limit, so x = 2 is not a vertical asymptote. ➤ 2.5 Limits at Infinity Limits at infinity—as opposed to infinite limits—occur when the independent variable becomes large in magnitude. For this reason, limits at infinity determine what is called the end behavior of a function. An application of these limits is to determine whether a sys- tem (such as an ecosystem or a large oscillating structure) reaches a steady state as time increases. Copyright © 2014 Pearson Education, Inc. For Use Only in 2013 2014– Pilot Program 2.5 Limits at Infinity 97 y lim f (x) q Limits at Infinity and Horizontal Asymptotes xᠬϱ 1 2 = -1 1- ∞ ∞2 q Consider the function f x tan x, whose domain is , (Figure 2.30). As S ∞ 1 2 p> x becomes arbitrarily large (denoted x ), f x approaches 2, and as x becomes Horizontal Ϫ1 S - ∞ 1 2 -p> f (x) tan x arbitrarily large in magnitude and negative (denoted x ), f x approaches 2. asymptote These limits are expressed as - p - p 2 x lim tan 1 x = and lim tan 1 x = - . xS∞ 2 xS-∞ 2 Horizontal asymptote The graph of f approaches the horizontal line y = p>2 as x S ∞, and it approaches the Ϫq horizontal line y = -p>2 as x S - ∞. These lines are called horizontal asymptotes. lim f (x) q xᠬϪϱ FIGURE 2.30 DEFINITION Limits at Infinity and Horizontal Asymptotes 1 2 y If f x becomes arbitrarily close to a finite number L for all sufficiently large and posi- lim f (x) L tive x, then we write xᠬϱ L 1 2 = lim f x L. S f (x) y ϭ f (x) x ∞ Ϫϱ 1 2 = x ៬ We say the limit of f x as x approaches infinity is L. In this case, the line y L is a horizontal asymptote of f (Figure 2.31). The limit at negative infinity, x x ϱ 1 2 = lim f x M, is defined analogously. When the limit exists, the horizontal ៬ xS - ∞ f (x) asymptote is y = M. M lim f (x) M xᠬϪϱ x ➤ FIGURE 2.31 QUICK CHECK 1 Evaluate x>1x + 12 for x = 10, 100, and 1000. What is lim ? xS∞ x + 1 EXAMPLE 1 Limits at infinity Evaluate the following limits. a + 10 b a + 3 sin x b a. lim 2 2 b. lim 3 ➤ The limit laws of Theorem 2.3 and the xS - ∞ x xS∞ 1x Squeeze Theorem apply if x S a is SOLUTION replaced with x S ∞ or x S - ∞. a. As x becomes large and negative, x2 becomes large and positive; in turn, 10>x2 y approaches 0. By the limit laws of Theorem 2.3, 10 10 10 f (x) 2 a + b = + a b = + = x2 lim 2 2 lim 2 lim 2 2 0 2. xS-∞ x xS-∞ (+xS+)++*-∞ x c equals 2 equals 0 lim f (x) 2 lim f (x) 2 10 xᠬϪϱ xᠬϱ Notice that lim a2 + b is also equal to 2. Therefore, the graph of y = 2 + 10>x2 xS∞ x2 = S ∞ S - ∞ 2 approaches the horizontal asymptote y 2 as x and as x (Figure 2.32). y ϭ 2 b. The numerator of sin x> 1x is bounded between -1 and 1; therefore, for x 7 0, x 2 1 sin x 1 - … … . FIGURE 2.32 1x 1x 1x As x S ∞, 1x becomes arbitrarily large, which means that -1 1 lim = lim = 0. xS∞ 1x xS∞ 1x sin x It follows by the Squeeze Theorem (Theorem 2.5) that lim = 0. xS∞ 1x Copyright © 2014 Pearson Education, Inc. For Use Only in 2013 2014– Pilot Program 98 Chapter 2 r Limits y Using the limit laws of Theorem 2.3, 6 3 sin x sin x lim a3 + b = lim 3 + 3 lim a b = 3. 3 sin x S∞ 1 S∞ S∞ 1 5 f (x) ϭ 3 ϩ x x x (+x +)++*x x e equals 3 equals 0 4 3 sin x 3 The graph of y = 3 + approaches the horizontal asymptote y = 3 as x 1x 2 lim f (x) 3 becomes large (Figure 2.33). Note that the curve intersects its asymptote infinitely x ϱ ➤ 1 ៬ many times. Related Exercises 9–14 0 0 1020 30 40 x Infinite Limits at Infinity FIGURE 2.33 It is possible for a limit to be both an infinite limit and a limit at infinity. This type of limit 1 2 occurs if f x becomes arbitrarily large in magnitude as x becomes arbitrarily large in lim f (x) magnitude. Such a limit is called an infinite limit at infinity and is illustrated by the func- xᠬϱ y 1 2 = 3 tion f x x (Figure 2.34). DEFINITION Infinite Limits at Infinity 1 1 2 f (x) ϭ x3 If f x becomes arbitrarily large as x becomes arbitrarily large, then we write 1 2 = ∞ lim f x . xS∞ Ϫ1 1 x 1 2 = - ∞ 1 2 = ∞ 1 2 = - ∞ The limits lim f x , lim f x , and lim f x are S∞ S - ∞ S - ∞ Ϫ x x x 1 defined similarly. Infinite limits at infinity tell us about the behavior of polynomials for large-magnitude lim f (x) 1 2 = n values of x. First, consider power functions f x x , where n is a positive integer. xᠬϪϱ Figure 2.35 shows that when n is even, lim xn = ∞, and when n is odd, lim xn = ∞ S { ∞ S∞ FIGURE 2.34 and lim xn = - ∞. x x xS - ∞ ϭ 5 n 0 even: y n 0 odd: y y x n n n lim x lim x lim x y ϭ x7 x ៬ Ϯϱ x ៬ ϱ x ៬ Ϫϱ 60 y ϭ x6 y ϭ x4 20 y ϭ x3 40 Ϫ3 Ϫ2 1 2 3 x 20 Ϫ20 y ϭ x2 Ϫ3 Ϫ2 Ϫ1 1 2 3 x FIGURE 2.35 Copyright © 2014 Pearson Education, Inc. For Use Only in 2013 2014– Pilot Program 2.5 Limits at Infinity 99 1 2 = > n = -n It follows that reciprocals of power functions f x 1 x x , where n is a positive integer, behave as follows: 1 = -n = 1 = -n = lim n lim x 0 and lim n lim x 0. xS∞ x xS∞ xS - ∞ x xS - ∞ S { ∞ QUICK CHECK 2 Describe the behavior From here, it is a short step to finding the behavior of any polynomial as x . Let 1 2 = n + n - 1 + g + 2 + + of p1x2 = -3x3 as x S ∞ and as p x anx an - 1x a2x a1x a0. We now write p in the equivalent x S - ∞. ➤ form a - a - a 1 2 = n ° + n 1 + n 2 + g+ 0 ¢ p x x an 2 n . x x "x e e S0 S0 S0 Notice that as x becomes large in magnitude, all the terms in p except the first term ap- S {∞ 1 2 ≈ n proach zero.
Recommended publications
  • Limits Involving Infinity (Horizontal and Vertical Asymptotes Revisited)
    Limits Involving Infinity (Horizontal and Vertical Asymptotes Revisited) Limits as ‘ x ’ Approaches Infinity At times you’ll need to know the behavior of a function or an expression as the inputs get increasingly larger … larger in the positive and negative directions. We can evaluate this using the limit limf ( x ) and limf ( x ) . x→ ∞ x→ −∞ Obviously, you cannot use direct substitution when it comes to these limits. Infinity is not a number, but a way of denoting how the inputs for a function can grow without any bound. You see limits for x approaching infinity used a lot with fractional functions. 1 Ex) Evaluate lim using a graph. x→ ∞ x A more general version of this limit which will help us out in the long run is this … GENERALIZATION For any expression (or function) in the form CONSTANT , this limit is always true POWER OF X CONSTANT lim = x→ ∞ xn HOW TO EVALUATE A LIMIT AT INFINITY FOR A RATIONAL FUNCTION Step 1: Take the highest power of x in the function’s denominator and divide each term of the fraction by this x power. Step 2: Apply the limit to each term in both numerator and denominator and remember: n limC / x = 0 and lim C= C where ‘C’ is a constant. x→ ∞ x→ ∞ Step 3: Carefully analyze the results to see if the answer is either a finite number or ‘ ∞ ’ or ‘ − ∞ ’ 6x − 3 Ex) Evaluate the limit lim . x→ ∞ 5+ 2 x 3− 2x − 5 x 2 Ex) Evaluate the limit lim . x→ ∞ 2x + 7 5x+ 2 x −2 Ex) Evaluate the limit lim .
    [Show full text]
  • Section 8.8: Improper Integrals
    Section 8.8: Improper Integrals One of the main applications of integrals is to compute the areas under curves, as you know. A geometric question. But there are some geometric questions which we do not yet know how to do by calculus, even though they appear to have the same form. Consider the curve y = 1=x2. We can ask, what is the area of the region under the curve and right of the line x = 1? We have no reason to believe this area is finite, but let's ask. Now no integral will compute this{we have to integrate over a bounded interval. Nonetheless, we don't want to throw up our hands. So note that b 2 b Z (1=x )dx = ( 1=x) 1 = 1 1=b: 1 − j − In other words, as b gets larger and larger, the area under the curve and above [1; b] gets larger and larger; but note that it gets closer and closer to 1. Thus, our intuition tells us that the area of the region we're interested in is exactly 1. More formally: lim 1 1=b = 1: b − !1 We can rewrite that as b 2 lim Z (1=x )dx: b !1 1 Indeed, in general, if we want to compute the area under y = f(x) and right of the line x = a, we are computing b lim Z f(x)dx: b !1 a ASK: Does this limit always exist? Give some situations where it does not exist. They'll give something that blows up.
    [Show full text]
  • The Infinity Theorem Is Presented Stating That There Is at Least One Multivalued Series That Diverge to Infinity and Converge to Infinite Finite Values
    Open Journal of Mathematics and Physics | Volume 2, Article 75, 2020 | ISSN: 2674-5747 https://doi.org/10.31219/osf.io/9zm6b | published: 4 Feb 2020 | https://ojmp.wordpress.com CX [microresearch] Diamond Open Access The infinity theorem Open Mathematics Collaboration∗† March 19, 2020 Abstract The infinity theorem is presented stating that there is at least one multivalued series that diverge to infinity and converge to infinite finite values. keywords: multivalued series, infinity theorem, infinite Introduction 1. 1, 2, 3, ..., ∞ 2. N =x{ N 1, 2,∞3,}... ∞ > ∈ = { } The infinity theorem 3. Theorem: There exists at least one divergent series that diverge to infinity and converge to infinite finite values. ∗All authors with their affiliations appear at the end of this paper. †Corresponding author: [email protected] | Join the Open Mathematics Collaboration 1 Proof 1 4. S 1 1 1 1 1 1 ... 2 [1] = − + − + − + = (a) 5. Sn 1 1 1 ... 1 has n terms. 6. S = lim+n + S+n + 7. A+ft=er app→ly∞ing the limit in (6), we have S 1 1 1 ... + 8. From (4) and (7), S S 2 = 0 + 2 + 0 + 2 ... 1 + 9. S 2 2 1 1 1 .+.. = + + + + + + 1 10. Fro+m (=7) (and+ (9+), S+ )2 2S . + +1 11. Using (6) in (10), limn+ =Sn 2 2 limn Sn. 1 →∞ →∞ 12. limn Sn 2 + = →∞ 1 13. From (6) a=nd (12), S 2. + 1 14. From (7) and (13), S = 1 1 1 ... 2. + = + + + = (b) 15. S 1 1 1 1 1 ... + 1 16. S =0 +1 +1 +1 +1 +1 1 ..
    [Show full text]
  • The Modal Logic of Potential Infinity, with an Application to Free Choice
    The Modal Logic of Potential Infinity, With an Application to Free Choice Sequences Dissertation Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Ethan Brauer, B.A. ∼6 6 Graduate Program in Philosophy The Ohio State University 2020 Dissertation Committee: Professor Stewart Shapiro, Co-adviser Professor Neil Tennant, Co-adviser Professor Chris Miller Professor Chris Pincock c Ethan Brauer, 2020 Abstract This dissertation is a study of potential infinity in mathematics and its contrast with actual infinity. Roughly, an actual infinity is a completed infinite totality. By contrast, a collection is potentially infinite when it is possible to expand it beyond any finite limit, despite not being a completed, actual infinite totality. The concept of potential infinity thus involves a notion of possibility. On this basis, recent progress has been made in giving an account of potential infinity using the resources of modal logic. Part I of this dissertation studies what the right modal logic is for reasoning about potential infinity. I begin Part I by rehearsing an argument|which is due to Linnebo and which I partially endorse|that the right modal logic is S4.2. Under this assumption, Linnebo has shown that a natural translation of non-modal first-order logic into modal first- order logic is sound and faithful. I argue that for the philosophical purposes at stake, the modal logic in question should be free and extend Linnebo's result to this setting. I then identify a limitation to the argument for S4.2 being the right modal logic for potential infinity.
    [Show full text]
  • 13 Limits and the Foundations of Calculus
    13 Limits and the Foundations of Calculus We have· developed some of the basic theorems in calculus without reference to limits. However limits are very important in mathematics and cannot be ignored. They are crucial for topics such as infmite series, improper integrals, and multi­ variable calculus. In this last section we shall prove that our approach to calculus is equivalent to the usual approach via limits. (The going will be easier if you review the basic properties of limits from your standard calculus text, but we shall neither prove nor use the limit theorems.) Limits and Continuity Let {be a function defined on some open interval containing xo, except possibly at Xo itself, and let 1 be a real number. There are two defmitions of the· state­ ment lim{(x) = 1 x-+xo Condition 1 1. Given any number CI < l, there is an interval (al> b l ) containing Xo such that CI <{(x) ifal <x < b i and x ;6xo. 2. Given any number Cz > I, there is an interval (a2, b2) containing Xo such that Cz > [(x) ifa2 <x< b 2 and x :;Cxo. Condition 2 Given any positive number €, there is a positive number 0 such that If(x) -11 < € whenever Ix - x 0 I< 5 and x ;6 x o. Depending upon circumstances, one or the other of these conditions may be easier to use. The following theorem shows that they are interchangeable, so either one can be used as the defmition oflim {(x) = l. X--->Xo 180 LIMITS AND CONTINUITY 181 Theorem 1 For any given f.
    [Show full text]
  • Cantor on Infinity in Nature, Number, and the Divine Mind
    Cantor on Infinity in Nature, Number, and the Divine Mind Anne Newstead Abstract. The mathematician Georg Cantor strongly believed in the existence of actually infinite numbers and sets. Cantor’s “actualism” went against the Aristote- lian tradition in metaphysics and mathematics. Under the pressures to defend his theory, his metaphysics changed from Spinozistic monism to Leibnizian volunta- rist dualism. The factor motivating this change was two-fold: the desire to avoid antinomies associated with the notion of a universal collection and the desire to avoid the heresy of necessitarian pantheism. We document the changes in Can- tor’s thought with reference to his main philosophical-mathematical treatise, the Grundlagen (1883) as well as with reference to his article, “Über die verschiedenen Standpunkte in bezug auf das aktuelle Unendliche” (“Concerning Various Perspec- tives on the Actual Infinite”) (1885). I. he Philosophical Reception of Cantor’s Ideas. Georg Cantor’s dis- covery of transfinite numbers was revolutionary. Bertrand Russell Tdescribed it thus: The mathematical theory of infinity may almost be said to begin with Cantor. The infinitesimal Calculus, though it cannot wholly dispense with infinity, has as few dealings with it as possible, and contrives to hide it away before facing the world Cantor has abandoned this cowardly policy, and has brought the skeleton out of its cupboard. He has been emboldened on this course by denying that it is a skeleton. Indeed, like many other skeletons, it was wholly dependent on its cupboard, and vanished in the light of day.1 1Bertrand Russell, The Principles of Mathematics (London: Routledge, 1992 [1903]), 304.
    [Show full text]
  • Two Fundamental Theorems About the Definite Integral
    Two Fundamental Theorems about the Definite Integral These lecture notes develop the theorem Stewart calls The Fundamental Theorem of Calculus in section 5.3. The approach I use is slightly different than that used by Stewart, but is based on the same fundamental ideas. 1 The definite integral Recall that the expression b f(x) dx ∫a is called the definite integral of f(x) over the interval [a,b] and stands for the area underneath the curve y = f(x) over the interval [a,b] (with the understanding that areas above the x-axis are considered positive and the areas beneath the axis are considered negative). In today's lecture I am going to prove an important connection between the definite integral and the derivative and use that connection to compute the definite integral. The result that I am eventually going to prove sits at the end of a chain of earlier definitions and intermediate results. 2 Some important facts about continuous functions The first intermediate result we are going to have to prove along the way depends on some definitions and theorems concerning continuous functions. Here are those definitions and theorems. The definition of continuity A function f(x) is continuous at a point x = a if the following hold 1. f(a) exists 2. lim f(x) exists xœa 3. lim f(x) = f(a) xœa 1 A function f(x) is continuous in an interval [a,b] if it is continuous at every point in that interval. The extreme value theorem Let f(x) be a continuous function in an interval [a,b].
    [Show full text]
  • Measuring Fractals by Infinite and Infinitesimal Numbers
    MEASURING FRACTALS BY INFINITE AND INFINITESIMAL NUMBERS Yaroslav D. Sergeyev DEIS, University of Calabria, Via P. Bucci, Cubo 42-C, 87036 Rende (CS), Italy, N.I. Lobachevsky State University, Nizhni Novgorod, Russia, and Institute of High Performance Computing and Networking of the National Research Council of Italy http://wwwinfo.deis.unical.it/∼yaro e-mail: [email protected] Abstract. Traditional mathematical tools used for analysis of fractals allow one to distinguish results of self-similarity processes after a finite number of iterations. For example, the result of procedure of construction of Cantor’s set after two steps is different from that obtained after three steps. However, we are not able to make such a distinction at infinity. It is shown in this paper that infinite and infinitesimal numbers proposed recently allow one to measure results of fractal processes at different iterations at infinity too. First, the new technique is used to measure at infinity sets being results of Cantor’s proce- dure. Second, it is applied to calculate the lengths of polygonal geometric spirals at different points of infinity. 1. INTRODUCTION During last decades fractals have been intensively studied and applied in various fields (see, for instance, [4, 11, 5, 7, 12, 20]). However, their mathematical analysis (except, of course, a very well developed theory of fractal dimensions) very often continues to have mainly a qualitative character and there are no many tools for a quantitative analysis of their behavior after execution of infinitely many steps of a self-similarity process of construction. Usually, we can measure fractals in a way and can give certain numerical answers to questions regarding fractals only if a finite number of steps in the procedure of their construction has been executed.
    [Show full text]
  • Calculus Terminology
    AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential
    [Show full text]
  • Attributes of Infinity
    International Journal of Applied Physics and Mathematics Attributes of Infinity Kiamran Radjabli* Utilicast, La Jolla, California, USA. * Corresponding author. Email: [email protected] Manuscript submitted May 15, 2016; accepted October 14, 2016. doi: 10.17706/ijapm.2017.7.1.42-48 Abstract: The concept of infinity is analyzed with an objective to establish different infinity levels. It is proposed to distinguish layers of infinity using the diverging functions and series, which transform finite numbers to infinite domain. Hyper-operations of iterated exponentiation establish major orders of infinity. It is proposed to characterize the infinity by three attributes: order, class, and analytic value. In the first order of infinity, the infinity class is assessed based on the “analytic convergence” of the Riemann zeta function. Arithmetic operations in infinity are introduced and the results of the operations are associated with the infinity attributes. Key words: Infinity, class, order, surreal numbers, divergence, zeta function, hyperpower function, tetration, pentation. 1. Introduction Traditionally, the abstract concept of infinity has been used to generically designate any extremely large result that cannot be measured or determined. However, modern mathematics attempts to introduce new concepts to address the properties of infinite numbers and operations with infinities. The system of hyperreal numbers [1], [2] is one of the approaches to define infinite and infinitesimal quantities. The hyperreals (a.k.a. nonstandard reals) *R, are an extension of the real numbers R that contains numbers greater than anything of the form 1 + 1 + … + 1, which is infinite number, and its reciprocal is infinitesimal. Also, the set theory expands the concept of infinity with introduction of various orders of infinity using ordinal numbers.
    [Show full text]
  • Notes Chapter 4(Integration) Definition of an Antiderivative
    1 Notes Chapter 4(Integration) Definition of an Antiderivative: A function F is an antiderivative of f on an interval I if for all x in I. Representation of Antiderivatives: If F is an antiderivative of f on an interval I, then G is an antiderivative of f on the interval I if and only if G is of the form G(x) = F(x) + C, for all x in I where C is a constant. Sigma Notation: The sum of n terms a1,a2,a3,…,an is written as where I is the index of summation, ai is the ith term of the sum, and the upper and lower bounds of summation are n and 1. Summation Formulas: 1. 2. 3. 4. Limits of the Lower and Upper Sums: Let f be continuous and nonnegative on the interval [a,b]. The limits as n of both the lower and upper sums exist and are equal to each other. That is, where are the minimum and maximum values of f on the subinterval. Definition of the Area of a Region in the Plane: Let f be continuous and nonnegative on the interval [a,b]. The area if a region bounded by the graph of f, the x-axis and the vertical lines x=a and x=b is Area = where . Definition of a Riemann Sum: Let f be defined on the closed interval [a,b], and let be a partition of [a,b] given by a =x0<x1<x2<…<xn-1<xn=b where xi is the width of the ith subinterval.
    [Show full text]
  • Calculus Formulas and Theorems
    Formulas and Theorems for Reference I. Tbigonometric Formulas l. sin2d+c,cis2d:1 sec2d l*cot20:<:sc:20 +.I sin(-d) : -sitt0 t,rs(-//) = t r1sl/ : -tallH 7. sin(A* B) :sitrAcosB*silBcosA 8. : siri A cos B - siu B <:os,;l 9. cos(A+ B) - cos,4cos B - siuA siriB 10. cos(A- B) : cosA cosB + silrA sirrB 11. 2 sirrd t:osd 12. <'os20- coS2(i - siu20 : 2<'os2o - I - 1 - 2sin20 I 13. tan d : <.rft0 (:ost/ I 14. <:ol0 : sirrd tattH 1 15. (:OS I/ 1 16. cscd - ri" 6i /F tl r(. cos[I ^ -el : sitt d \l 18. -01 : COSA 215 216 Formulas and Theorems II. Differentiation Formulas !(r") - trr:"-1 Q,:I' ]tra-fg'+gf' gJ'-,f g' - * (i) ,l' ,I - (tt(.r))9'(.,') ,i;.[tyt.rt) l'' d, \ (sttt rrJ .* ('oqI' .7, tJ, \ . ./ stll lr dr. l('os J { 1a,,,t,:r) - .,' o.t "11'2 1(<,ot.r') - (,.(,2.r' Q:T rl , (sc'c:.r'J: sPl'.r tall 11 ,7, d, - (<:s<t.r,; - (ls(].]'(rot;.r fr("'),t -.'' ,1 - fr(u") o,'ltrc ,l ,, 1 ' tlll ri - (l.t' .f d,^ --: I -iAl'CSllLl'l t!.r' J1 - rz 1(Arcsi' r) : oT Il12 Formulas and Theorems 2I7 III. Integration Formulas 1. ,f "or:artC 2. [\0,-trrlrl *(' .t "r 3. [,' ,t.,: r^x| (' ,I 4. In' a,,: lL , ,' .l 111Q 5. In., a.r: .rhr.r' .r r (' ,l f 6. sirr.r d.r' - ( os.r'-t C ./ 7. /.,,.r' dr : sitr.i'| (' .t 8. tl:r:hr sec,rl+ C or ln Jccrsrl+ C ,f'r^rr f 9.
    [Show full text]